## Electromagnetic fieldsThis revised edition provides patient guidance in its clear and organized presentation of problems. It is rich in variety, large in number and provides very careful treatment of relativity. One outstanding feature is the inclusion of simple, standard examples demonstrated in different methods that will allow students to enhance and understand their calculating abilities. There are over 145 worked examples; virtually all of the standard problems are included. |

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Page 143

The subscript b appearing in (10-7), (10-8), and (10-10) reflects the fact that these

charge densities arise from the

they are usually referred to as the

The subscript b appearing in (10-7), (10-8), and (10-10) reflects the fact that these

charge densities arise from the

**bound charges**of the dielectric. Consequently,they are usually referred to as the

**bound charge**densities or the polarization ...Page 168

(a) Find the

points on the z axis for which z > 0. (c) Verify that your results in (b) satisfy the

boundary condition at z — L. (d) From the result of (b), find E at the origin, (e)

Sketch ...

(a) Find the

**bound charge**densities pb and ab. (b) Find the electric field for allpoints on the z axis for which z > 0. (c) Verify that your results in (b) satisfy the

boundary condition at z — L. (d) From the result of (b), find E at the origin, (e)

Sketch ...

Page 206

equal the rate at which the total charge within V is decreasing, since the total

must be constant. ... Now in the process of polarizing a material, the

define a ...

equal the rate at which the total charge within V is decreasing, since the total

must be constant. ... Now in the process of polarizing a material, the

**bound****charges**will generally be moving, as we saw in Section 10-1, so that we candefine a ...

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angle assume axes axis becomes bound charge boundary conditions bounding surface calculate capacitance cavity charge density charge distribution charge q circuit conducting conductor const constant corresponding Coulomb's law current density curve cylinder dielectric dipole direction displacement distance divergence theorem electric field electromagnetic electrostatic energy equal equipotential evaluate example Exercise expression field point flux free charge function given illustrated in Figure induction infinitely long integral integrand Laplace's equation line charge located Lorentz transformation magnetic magnitude Maxwell's equations normal component obtained origin parallel plate capacitor particle perpendicular point charge polarized position vector potential difference quadrupole quantities rectangular coordinates region result satisfy scalar potential shown in Figure situation solenoid solution sphere of radius spherical surface charge surface charge density surface integral tangential components theorem total charge vacuum vector potential velocity volume write written xy plane zero